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Eternal life of entropy in non-Hermitian quantum systems

机译:非封闭型量子系统的熵永生

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We find a different effect for the behavior of von Neumann entropy. For this we derive the framework for describing von Neumann entropy in non-Hermitian quantum systems and then apply it to a simple interacting PT -symmetric bosonic system. We show that our model is well defined even in the PT -broken regime with the introduction of a time-dependent metric and that it displays three distinct behaviors relating to the PT symmetry of the original time-independent Hamiltonian.When the symmetry is unbroken, the entropy undergoes rapid decay to zero (so-called "sudden death") with a subsequent revival. At the exceptional point it decays asymptotically to zero and when the symmetry is spontaneously broken it decays asymptotically to a finite constant value ("eternal life").
机译:我们为von Neumann熵的行为达到了不同的效果。 为此,我们推出了描述非封闭型量子系统中的von Neumann熵的框架,然后将其应用于简单的相互作用的Pt -symmetric Bosonic系统。 我们表明,即使在PT -BROKER制度中,我们的模型也在引入时间依赖的公制,并且它显示出与原始时间独立的Hamiltonian的PT对称相关三个不同的行为。当对称性不间断时, 熵经历快速衰减到零(所谓的“突然死亡”)随后的复兴。 在卓越的点处,它衰减到零,当对称性自发地破裂时,它衰减渐近,以有限恒定值(“永生”)。

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